Modal parameter identification method for bounded and related uncertainty structure

By applying convex set theory and perturbation theory in modal parameter recognition, the correlation matrix of uncertain parameters is constructed and the second-order singular value decomposition is solved, and the traditional method's problem of degradation of recognition accuracy and high computing resource consumption is achieved when dealing with structural uncertainty, and more accurate and efficient modal parameter recognition is achieved.

CN119557959AActive Publication Date: 2025-03-04BEIHANG UNIV
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Patent Information

Application Number
CN202411727246.9
Authority / Receiving Office
CN · China
Patent Type
Applications(China)
Current Assignee / Owner
Filing Date
2024-11-28
Publication Date
2025-03-04
Estimated Expiration
2044-11-28

AI Technical Summary

Technical Problem

When traditional modal parameter recognition methods deal with structural uncertainty and various uncertainty factors, there are problems such as decreasing identification accuracy and high computing resource consumption.

Method used

Convex set theory and perturbation theory are used to construct a correlation matrix between uncertain parameters, generate a new uncertainty boundary, and analyze the propagation law of uncertainty in the singular value decomposition process through the second-order singular value decomposition method for convex sets, and obtain the uncertainty identification result of modal parameters.

Benefits of technology

Effectively quantify and deal with structural uncertainty and its correlation, reduce deviations in the modal parameter identification process, provide more accurate modal parameter estimation, and reduce the calculation amount and time required.

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Abstract

The invention relates to a modal parameter identification method for a bounded and related uncertainty structure, and belongs to the technical field of modal parameter identification and structure health monitoring. According to the method provided by the invention, the propagation rule of the structural parameter convex set uncertainty is deduced, and a general solving method is provided for parameter identification work under the influence of the convex set uncertainty. According to the method, the correlation between structural uncertainty factors is considered, and compared with an identification method which independently considers the uncertainty of each factor, the method is more scientific and higher in applicability; in addition, a second-order convex set singular value decomposition algorithm and a second-order convex set eigenvalue decomposition algorithm are provided, compared with a first-order method, through second-order Taylor expansion of singular values and eigenvalues, a more accurate singular value second-order interval estimation result and an accurate eigenvalue second-order interval estimation result are obtained, and the method has the advantages of being high in accuracy and high in robustness. And more accurate estimation results of modal parameters such as natural frequency and damping ratio can be obtained.
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Description

Technical Field

[0001] The present invention is applicable to the problem of structural uncertainty identification, belongs to the fields of modal parameter identification, structural health monitoring, etc., and specifically relates to a modal parameter identification method for a structure with bounded and correlated uncertainties. Background Art

[0002] With the continuous advancement of modern engineering technology, the complexity and dynamic characteristics of buildings and infrastructure have become increasingly significant, and the dynamic response of structures has become increasingly important to ensure their safety and reliability. In recent years, the influence of natural factors such as earthquakes and wind loads has led to a sharp increase in the demand for structural health monitoring systems and damage identification technologies. Effective modal parameter identification can not only help engineers understand the behavior of structures under dynamic loads, but also provide an important basis for the maintenance and reinforcement of structures. Therefore, accurately identifying the modal parameters of structures (such as frequency, damping ratio, etc.) has become a core task in structural dynamics research.

[0003] Traditional modal parameter identification methods, such as the ERA algorithm, perform well in multiple-input multiple-output (MIMO) systems. ERA can extract the modal characteristics of the structure from the input and output data by performing eigenvalue analysis on the system state space equations. However, ERA often encounters the problem of reduced identification accuracy when dealing with high-dimensional data and in the presence of noise. Measurement noise may lead to the appearance of pseudo-modes, which in turn affects the accuracy of modal parameters. In addition, the ERA method has high requirements on the dimension of the matrix during the calculation process. When dealing with large structures, the consumption of computing resources also becomes a major bottleneck.

[0004] To overcome these limitations, the ERA / DC method was developed. ERA / DC optimizes the computational efficiency of the algorithm by introducing the correlated Hankel matrix instead of the generalized Hankel matrix. This method reduces the computational complexity while improving the noise resistance. However, with the increasing complexity of the structural model, the uncertainty of environmental and material parameters has become increasingly prominent. These uncertainties may come from a variety of factors, including changes in material properties, differences in construction processes, and fluctuations in environmental conditions. These factors not only increase the difficulty of modal parameter identification, but may also lead to inaccurate structural safety assessment results.

[0005] In this context, researchers have gradually realized the shortcomings of traditional identification methods in dealing with uncertainty in view of the impact of uncertainty on modal parameter identification. Many studies have shown that ignoring the correlation and uncertainty between parameters will lead to deviations in the results. Therefore, establishing an effective mathematical model to describe these uncertainties has become the key to improving the accuracy of modal parameter identification. In recent years, convex set theory has shown good results in describing uncertainty because it considers the correlation between uncertainty parameters. By constructing an uncertainty model based on convex sets, researchers can consider the relationship between different parameters more comprehensively, thereby providing a more reliable basis for modal parameter identification.

[0006] While considering structural uncertainty, uncertainty also runs through the entire identification process, affecting the final identification accuracy. The perturbation method overcomes the limitations of traditional methods in high-dimensional data and uncertainty. This method not only focuses on the accurate identification of modal parameters, but also considers the variation law of parameters under the influence of uncertainty. Only a small amount of information such as the upper and lower bounds of structural uncertainty is needed to further solve the identification result interval, greatly reducing the amount of calculation and the time required. Summary of the invention

[0007] The purpose of the present invention is to overcome the problems of inaccurate identification caused by structural uncertainty and the correlation between uncertainty factors, and propose a modal parameter identification method for a structure with bounded and correlated uncertainties.

[0008] The technical solution of the present invention is as follows: first, a convex set is used to quantify structural uncertainty, and correlation is added on the basis of the original independent consideration of uncertainty boundary pairs to generate a new uncertainty boundary; then, a dynamic model of the structure is established to obtain the discretized state space equation, response function and generalized Hankel matrix, and the propagation of convex set uncertainty is considered in this process; then, based on perturbation theory, a second-order singular value decomposition method for convex sets is proposed, which analyzes the propagation law of convex set uncertainty in the singular value decomposition process and obtains the singular value boundary estimation after singular value decomposition. Finally, the system matrix required for identification is obtained, and a second-order eigenvalue decomposition is performed to obtain the boundary estimation of the eigenvalue, and then the modal parameter interval is obtained based on the eigenvalue boundary estimation.

[0009] The specific technical solution of the present invention is: a modal parameter identification method for a structure with bounded and correlated uncertainties, the steps of the method comprising:

[0010] Step 1: Determine the uncertainty parameters and their uncertainty ranges in the structural parameters;

[0011] Step 2: Construct the correlation matrix between uncertainty parameters, and construct the uncertainty parameter expression in convex set form according to the uncertainty range of the parameters and the correlation matrix, which is the convex set uncertainty;

[0012] Step 3: Construct a dynamic model of the structure and calculate the partial derivatives after the convex set uncertainty propagation in the dynamic model;

[0013] Step 4: Discretize the state space of the dynamic model of the structure in step 3 to obtain a discrete-time, time-invariant, linear dynamic system state parameter equation group, and then obtain the system matrix, input matrix and output matrix based on the obtained dynamic system state parameter equation group, and calculate the partial derivative form and uncertainty boundary of the system matrix and input matrix with respect to the uncertainty parameters;

[0014] Step 5: Calculate the response function under unit pulse excitation according to the system matrix, input matrix and output matrix obtained in step 4, then construct the generalized Hankel matrix according to the response function of each time interval, and calculate the partial derivative form of the generalized Hankel matrix with respect to the uncertainty parameter;

[0015] Step 6: According to the partial derivative form of the generalized Hankel matrix with respect to the convex set uncertainty parameters obtained in step 5, introduce it into the second-order convex set singular value decomposition process of the generalized Hankel matrix to obtain the convex set uncertainty estimation form of the singular values ​​and the first-order and second-order partial derivative forms of the convex set uncertainty parameters, the convex set uncertainty estimation form of the left and right singular value vectors and the first-order and second-order partial derivative forms of the convex set uncertainty parameters;

[0016] Step 7: Obtain the generalized Hankel matrix after time lapse according to the generalized Hankel matrix obtained in step 5;

[0017] Step 8: Construct the structure identification system matrix according to the time-shifted generalized Hankel matrix obtained in step 7 and the convex set uncertainty estimation form of the singular values ​​and left and right singular vectors obtained in step 6, and calculate the partial derivative form of the structure identification system matrix with respect to the convex set uncertainty parameters;

[0018] Step 9: Perform a second-order convex set eigenvalue decomposition on the structure identification system matrix obtained in step 8 to obtain the convex set uncertainty estimation form of the complex eigenvalue and the first-order and second-order partial derivative forms of the complex eigenvalue with respect to the uncertainty parameters, including the convex set uncertainty estimation form of the real part and imaginary part of the complex eigenvalue and the partial derivative forms of the two with respect to the uncertainty parameters;

[0019] Step 10: Calculate the modal parameters of the structure based on the convex set uncertainty estimation form of the complex eigenvalues ​​obtained in step 9 and the first-order and second-order partial derivative forms of the uncertainty parameters, obtain the uncertainty identification results of the natural frequency and damping ratio modal parameters of the structure, and perform structural health detection, fault diagnosis and dynamic control.

[0020] The present invention has the beneficial effects:

[0021] 1. The present invention can comprehensively consider the mutual influence between different uncertainty factors by constructing a correlation matrix between uncertainty parameters, making the identification of modal parameters more scientific.

[0022] 2. By introducing convex set theory, the present invention can effectively quantify and process structural uncertainties and their correlations, thereby reducing the deviation in the modal parameter identification process and providing more accurate modal parameter estimation.

[0023] 3. The present invention adopts perturbation theory, and only needs a small amount of information about the upper and lower bounds of uncertainty to perform interval solution of modal parameters, which significantly reduces the amount of calculation and the time required, and has more advantages in engineering applications.

[0024] 4. Based on perturbation theory, the present invention proposes a second-order singular value decomposition algorithm for convex sets. Through the second-order Taylor expansion, a more accurate singular value boundary estimation is obtained compared with the first-order singular value decomposition.

[0025] 5. This method is suitable for the identification of structural modal parameters in a variety of complex environments and conditions, especially in the identification of large-scale structural modal parameters, it is more accurate than the identification method that does not consider the correlation. BRIEF DESCRIPTION OF THE DRAWINGS

[0026] Figure 1 It is a schematic diagram of the method flow of the present invention;

[0027] Figure 2 This is a schematic diagram of a four-layer frame structure. DETAILED DESCRIPTION

[0028] In order to make the purpose, technical scheme and advantages of the present invention more clearly understood, the present invention is further described in detail below in conjunction with the accompanying drawings and embodiments. It should be understood that the specific embodiments described herein are only used to explain the present invention and are not intended to limit the present invention. In addition, the technical features involved in each embodiment of the present invention described below can be combined with each other as long as they do not conflict with each other. To achieve the above-mentioned purpose, the present invention adopts the following technical scheme.

[0029] Figure 1 A flow chart of a modal parameter identification method for a structure with bounded and correlated uncertainties proposed by the present invention, comprising the following steps:

[0030] Step 1: Determine the uncertainty parameters and their uncertainty ranges in the structural parameters;

[0031] Step 2: Construct the correlation matrix between uncertainty parameters, and construct the uncertainty parameter expression in convex set form according to the uncertainty range of the parameters and the correlation matrix, which is the convex set uncertainty;

[0032] Step 3: Construct a dynamic model of the structure and calculate the partial derivatives after the convex set uncertainty propagation in the dynamic model;

[0033] Step 4: Discretize the state space of the dynamic model of the structure in step 3 to obtain a discrete-time, time-invariant, linear dynamic system state parameter equation group, and then obtain the system matrix, input matrix and output matrix based on the obtained dynamic system state parameter equation group, and calculate the partial derivative form and uncertainty boundary of the system matrix and input matrix with respect to the uncertainty parameters;

[0034] Step 5: Calculate the response function under unit pulse excitation according to the system matrix, input matrix and output matrix obtained in step 4, then construct the generalized Hankel matrix according to the response function of each time interval, and calculate the partial derivative form of the generalized Hankel matrix with respect to the uncertainty parameter;

[0035] Step 6: According to the partial derivative form of the generalized Hankel matrix with respect to the convex set uncertainty parameters obtained in step 5, introduce it into the second-order convex set singular value decomposition process of the generalized Hankel matrix to obtain the convex set uncertainty estimation form of the singular values ​​and the first-order and second-order partial derivative forms of the convex set uncertainty parameters, the convex set uncertainty estimation form of the left and right singular value vectors and the first-order and second-order partial derivative forms of the convex set uncertainty parameters;

[0036] Step 7: Obtain the generalized Hankel matrix after time lapse according to the generalized Hankel matrix obtained in step 5;

[0037] Step 8: Construct the structure identification system matrix according to the time-shifted generalized Hankel matrix obtained in step 7 and the convex set uncertainty estimation form of the singular values ​​and left and right singular vectors obtained in step 6, and calculate the partial derivative form of the structure identification system matrix with respect to the convex set uncertainty parameters;

[0038] Step 9: Perform a second-order convex set eigenvalue decomposition on the structure identification system matrix obtained in step 8 to obtain the convex set uncertainty estimation form of the complex eigenvalue and the first-order and second-order partial derivative forms of the complex eigenvalue with respect to the uncertainty parameters, including the convex set uncertainty estimation form of the real part and imaginary part of the complex eigenvalue and the partial derivative forms of the two with respect to the uncertainty parameters;

[0039] Step 10: Calculate the modal parameters of the structure based on the convex set uncertainty estimation form of the complex eigenvalues ​​obtained in step 9 and the first-order and second-order partial derivative forms of the uncertainty parameters, obtain the uncertainty identification results of the natural frequency and damping ratio modal parameters of the structure, and perform structural health detection, fault diagnosis and dynamic control.

[0040] Further, in step 1, the uncertainty of the structural parameters is determined as follows:

[0041] ,

[0042] in, represents the uncertainty vector, which is composed of uncertainty parameters composition, represents the lower and upper bounds of the uncertainty vector when the correlation between uncertainty parameters is not considered, represents the central value vector of the uncertainty vector, represents the radius vector of the uncertainty vector, Indicates the standard uncertainty range , the total number of uncertainty parameters is , each uncertainty parameter is expressed as a central value and radius The combination form of Indicates The uncertainty parameters are related to the superscript Indicates the parameter center value.

[0043] Further, in step 2, the correlation matrix between the uncertainty parameters is constructed as follows:

[0044] ,

[0045] in, represents the correlation matrix between uncertainty parameters, Indicates The uncertainty parameter is related to The covariance between the uncertainty parameters, Indicates The uncertainty parameter is related to The correlation coefficient between the uncertainty parameters.

[0046] Furthermore, in step 2, the uncertainty parameters are expressed as a convex set form according to the parameter uncertainty and correlation matrix:

[0047] ,

[0048] in, represents a convex set.

[0049] Further, in step 3, the dynamic model of the structure is constructed as:

[0050] ,

[0051] in, denote the displacement, velocity and acceleration vectors respectively, represents the external load, is the structural mass matrix, is the structural stiffness matrix, is the structural damping matrix, which obeys the Rayleigh damping form, that is, , is the Rayleigh damping coefficient, which is determined according to the set damping ratio.

[0052] Further, in step 3, the structural mass matrix in the structural dynamics model is calculated For each uncertainty parameter Modified partial derivatives , structural stiffness matrix Partial derivatives with respect to uncertain parameters , structural damping matrix Partial derivatives with respect to uncertain parameters They are:

[0053] (1) Structural mass matrix Performing a first-order Taylor expansion, we get:

[0054] ,

[0055] in, ;

[0056] The above formula, Represents the mass matrix Partial derivatives of uncertain parameters;

[0057] (2) Structural stiffness matrix Performing a first-order Taylor expansion, we get:

[0058] ,

[0059] in, ;

[0060] The above formula, Represents the stiffness matrix For Partial derivatives of uncertain parameters;

[0061] (3) Structural damping matrix Performing a first-order Taylor expansion, we get:

[0062] ,

[0063] in, ;

[0064] The above formula, Represents the stiffness matrix For Partial derivatives of uncertain parameters.

[0065] Furthermore, in step 4, the state space of the constructed structural dynamics model is:

[0066] ,

[0067] in, represents the state variable, represents the output variable, represents the input variable, They represent the system matrix, input matrix and output matrix in continuous time respectively, and are calculated by the following formula:

[0068] ,

[0069] in, Represents the identity matrix.

[0070] Further, in step 4, the discretized state space is:

[0071] ,

[0072] in, represents the current sampling time, They represent the system matrix and input matrix in discrete time, respectively, and are calculated by the following formula:

[0073] ,

[0074] in, is the sampling time interval, the discretized output matrix It is consistent with the representation in continuous time; the system matrix after discretization is and the input matrix For uncertain parameters The partial derivatives are:

[0075] ,

[0076] In a convex set, the system matrix There are the following relationships:

[0077] ,

[0078] in, represents a convex set, is the system matrix Middle Line The convex set of column elements is calculated as follows:

[0079] ,

[0080] in, Representation matrix Middle Line Nominal values ​​of column elements; orthogonal matrix and the diagonal matrix Obtained by Cholesky decomposition: ; represents the hyperellipsoid formed by the initial convex set uncertainty parameters; yes Bias vector for each uncertainty parameter:

[0081] ; express Convex set perturbation of ;

[0082] Through convex set uncertainty, we know The boundary of is calculated by the following formula:

[0083] ,

[0084] In step 4, the uncertainty range of the system matrix and the input matrix is:

[0085] .

[0086] Furthermore, in step 5, the system response function under unit pulse excitation is for:

[0087] ,

[0088] Construct the generalized Hankel matrix as:

[0089] ,

[0090] in, and They represent the number of row blocks and column blocks of the generalized Hankel matrix respectively;

[0091] In step 5, the partial derivative of the generalized Hankel matrix with respect to the uncertainty parameter is calculated:

[0092] ,

[0093] in, .

[0094] Furthermore, in step 6, the generalized Hankel matrix considering parameter correlation is Perform a second-order singular value decomposition:

[0095] ,

[0096] in, denote the left singular value matrix and the right singular value matrix respectively, Respectively represent Column left singular value vector and Column right singular value vector:

[0097] ,

[0098] in, is the mode number of interest; , , They represent the center value of the left singular value vector and the uncertainty range of the left singular value vector after the first-order and second-order Taylor expansion respectively; , , They represent the central value of the right singular value vector and the uncertainty range of the right singular value vector after the first-order and second-order Taylor expansion respectively;

[0099] is the singular value matrix, Indicates singular values; ,

[0100] In the formula, , , They represent the central value of the singular value and the uncertainty range of the singular value after the first-order and second-order Taylor expansion respectively;

[0101] The radius after the first-order Taylor expansion is calculated by the following formula:

[0102] ,

[0103] in, express Bias vector for each uncertainty parameter:

[0104] ,

[0105] express Bias vector for each uncertainty parameter:

[0106] ,

[0107] express Bias vector for each uncertainty parameter:

[0108] ,

[0109] The uncertainty range after the second-order Taylor expansion is calculated by the following formula:

[0110] ,

[0111] According to the propagation of convex set uncertainty, we have:

[0112] ,

[0113] in, They represent the partial derivative of the left singular value vector with respect to the uncertainty parameter and the partial derivative of the right singular value vector with respect to the interval uncertainty parameter, respectively, and are calculated by the following formula:

[0114] ,

[0115] in, Indicates The left singular value vector elements, Indicates The right singular value vector elements.

[0116] Furthermore, in step 7, the generalized Hankel matrix after time elapses is for:

[0117] .

[0118] Furthermore, in step 8, the structure recognition system matrix constructed for:

[0119] ,

[0120] in, ;

[0121] Structure Identification System Matrix The partial derivative with respect to the uncertainty parameter is:

[0122] ,

[0123] Further, in step 9, the structure identification system matrix The second-order convex set eigenvalue decomposition is:

[0124] ,

[0125] in, is the eigenvalue vector, represents the complex eigenvalue matrix, Indicates Item complex eigenvalue;

[0126] , ,

[0127] ,

[0128] Among them, the first-order partial derivative of the complex eigenvalue with respect to the uncertainty parameter And the second-order partial derivative The calculation is as follows:

[0129] ,

[0130] ,

[0131] Among them, the first-order partial derivative of the eigenvalue vector with respect to the uncertainty parameter for:

[0132] ,

[0133] .

[0134] Further, in step 10, the modal parameters of the structure calculated are:

[0135] Natural circular frequency for: ,

[0136] in, They represent the central value of the natural frequency, the uncertainty range of the natural frequency, and the lower and upper limits of the range, respectively. The expression is ;

[0137] The upper and lower bounds are determined as follows:

[0138] Will The expression is regarded as The quadratic function of is a variable with a range, we get exist The minimum and maximum values ​​within the range of variation are the lower and upper bounds, and the calculation process is as follows:

[0139] ,

[0140] ,

[0141] in, represents the uncertainty parameter of the i-th natural frequency with respect to the j-th uncertainty parameter The uncertainty range of

[0142] Among them, the first-order and second-order partial derivatives of the natural circular frequency with respect to the uncertainty parameter are as follows:

[0143] ,

[0144] ,

[0145] in, Represents complex eigenvalues The partial derivatives of the real and imaginary parts of the uncertainty parameter are calculated by the following formula:

[0146] ,

[0147] ,

[0148] Damping ratio range for: ;

[0149] in, They represent the central value of the damping ratio, the uncertainty range of the damping ratio, and the lower and upper bounds, respectively. The expression is ;

[0150] The upper and lower bounds are determined as follows:

[0151] Will The expression is regarded as The quadratic function of is a variable with a range, we get exist The minimum and maximum values ​​within the range of variation are the lower and upper bounds, and the calculation process is as follows:

[0152] ,

[0153] ,

[0154] in, represents the uncertainty parameter of the i-th natural frequency with respect to the j-th uncertainty parameter The uncertainty range of

[0155] Among them, the first-order and second-order partial derivatives of the damping ratio with respect to the uncertainty parameter are as follows:

[0156] ,

[0157] .

[0158] Further, step 1: determine the uncertain parameters and parameter uncertainties in the structural parameters; specifically:

[0159] like Figure 2 As shown in the figure, a four-story frame structure is used as the basic example, assuming that the structural quality and stiffness Structural parameters such as are affected by processing conditions and working scenarios and are uncertain, and are expressed in the form of interval vectors as follows:

[0160]

[0161] in, Indicates the standard uncertainty range ; The uncertainty vectors representing the structural mass and structural stiffness are The lower and upper bounds of the uncertainty vector The uncertainty parameters composition, which can be expressed as the median and radius The number of uncertainty parameters is .

[0162] The material density of the structure is , Young's modulus is The cross-sectional areas of the four beams are , , , The cross-sectional area of ​​the cylinder is The mass and stiffness of the final model have an uncertainty of 2%.

[0163] Step 10, the uncertainty identification results of modal parameters such as the natural frequency and damping ratio of the structure are shown in the following table:

[0164]

[0165] In this way, parameters such as the natural frequency of the structure are obtained. According to the obtained modal parameters, a theoretical model can be provided for the design of the structural controller, and it can also be used as an important parameter for structural health monitoring.

[0166] In summary, the above are only preferred embodiments of the present invention and are not intended to limit the protection scope of the present invention. Any modifications, equivalent substitutions, improvements, etc. made within the spirit and principles of the present invention should be included in the protection scope of the present invention.

Claims

1. A method for modal parameter identification of a structure with bounded and correlated uncertainties, characterized in that: The steps of the method include: Step 1: Determine the uncertainty parameters and their uncertainty ranges in the structural parameters; Step 2: Construct the correlation matrix between uncertainty parameters, and construct the uncertainty parameter expression in convex set form according to the uncertainty range of the parameters and the correlation matrix, which is the convex set uncertainty; Step 3: Construct a dynamic model of the structure and calculate the partial derivatives after the convex set uncertainty propagation in the dynamic model; Step 4: Discretize the state space of the dynamic model of the structure in step 3 to obtain a discrete-time, time-invariant, linear dynamic system state parameter equation group, and then obtain the system matrix, input matrix and output matrix based on the obtained dynamic system state parameter equation group, and calculate the partial derivative form and uncertainty boundary of the system matrix and input matrix with respect to the uncertainty parameters; Step 5: Calculate the response function under unit pulse excitation according to the system matrix, input matrix and output matrix obtained in step 4, then construct the generalized Hankel matrix according to the response function of each time interval, and calculate the partial derivative form of the generalized Hankel matrix with respect to the uncertainty parameter; Step 6: According to the partial derivative form of the generalized Hankel matrix with respect to the convex set uncertainty parameters obtained in step 5, introduce it into the second-order convex set singular value decomposition process of the generalized Hankel matrix to obtain the convex set uncertainty estimation form of the singular values ​​and the first-order and second-order partial derivative forms of the convex set uncertainty parameters, the convex set uncertainty estimation form of the left and right singular value vectors and the first-order and second-order partial derivative forms of the convex set uncertainty parameters; Step 7: Obtain the generalized Hankel matrix after time lapse according to the generalized Hankel matrix obtained in step 5; Step 8: Construct the structure identification system matrix according to the time-shifted generalized Hankel matrix obtained in step 7 and the convex set uncertainty estimation form of the singular values ​​and left and right singular vectors obtained in step 6, and calculate the partial derivative form of the structure identification system matrix with respect to the convex set uncertainty parameters; Step 9: Perform a second-order convex set eigenvalue decomposition on the structure identification system matrix obtained in step 8 to obtain the convex set uncertainty estimation form of the complex eigenvalue and the first-order and second-order partial derivative forms of the complex eigenvalue with respect to the uncertainty parameters, including the convex set uncertainty estimation form of the real part and imaginary part of the complex eigenvalue and the partial derivative forms of the two with respect to the uncertainty parameters; Step 10: Calculate the modal parameters of the structure based on the convex set uncertainty estimation form of the complex eigenvalues ​​obtained in step 9 and the first-order and second-order partial derivative forms of the uncertainty parameters, obtain the uncertainty identification results of the natural frequency and damping ratio modal parameters of the structure, and perform structural health detection, fault diagnosis and dynamic control.

2. A method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 1, characterized in that: In step 1, the uncertainties in the structural parameters are determined as follows: , in, represents the uncertainty vector, which is composed of uncertainty parameters composition, represents the lower and upper bounds of the uncertainty vector when the correlation between uncertainty parameters is not considered, represents the central value vector of the uncertainty vector, represents the radius vector of the uncertainty vector, Indicates the standard uncertainty range , the total number of uncertainty parameters is , each uncertainty parameter is expressed as a central value and radius The combination form of Indicates The uncertainty parameters are related to the superscript Indicates the parameter center value.

3. The method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 2, characterized in that: In step 2, the correlation matrix between uncertainty parameters is constructed as follows: , in, represents the correlation matrix between uncertainty parameters, Indicates The uncertainty parameter is related to The covariance between the uncertainty parameters, Indicates The uncertainty parameter is related to The correlation coefficient between the uncertainty parameters.

4. A method for identifying modal parameters of a structure with bounded and correlated uncertainties according to claim 3, characterized in that: In step 2, the uncertainty parameters are expressed as a convex set form based on the parameter uncertainty and correlation matrix: , in, represents a convex set.

5. A method for identifying modal parameters of a structure with bounded and correlated uncertainties according to claim 4, characterized in that: In step 3, the dynamic model of the structure is constructed as: , in, denote the displacement, velocity and acceleration vectors respectively, represents the external load, is the structural mass matrix, is the structural stiffness matrix, is the structural damping matrix, which obeys the Rayleigh damping form, that is, , is the Rayleigh damping coefficient, which is determined according to the set damping ratio.

6. A method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 5, characterized in that: In step 3, the structural mass matrix of the structural dynamics model is calculated For each uncertainty parameter Modified partial derivatives , structural stiffness matrix Partial derivatives with respect to uncertain parameters , structural damping matrix Partial derivatives with respect to uncertain parameters They are: (1) Structural mass matrix Performing a first-order Taylor expansion, we get: , in, ; The above formula, Represents the mass matrix Partial derivatives of uncertain parameters; (2) Structural stiffness matrix Performing a first-order Taylor expansion, we get: , in, , The above formula, Represents the stiffness matrix For Partial derivatives of uncertain parameters; (3) Structural damping matrix Performing a first-order Taylor expansion, we get: , in, , The above formula, Represents the stiffness matrix For Partial derivatives of uncertain parameters.

7. A method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 6, characterized in that: In step 4, the state space of the constructed structural dynamics model is: , in, represents the state variable, represents the output variable, represents the input variable, They represent the system matrix, input matrix and output matrix in continuous time respectively, and are calculated by the following formula: , in, Represents the identity matrix.

8. A method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 7, characterized in that: In step 4, the discretized state space is: , in, Represents the current sampling time, They represent the system matrix and input matrix in discrete time, respectively, and are calculated by the following formula: , in, is the sampling time interval, the discretized output matrix It is consistent with the representation in continuous time; the system matrix after discretization is and the input matrix For uncertain parameters The partial derivatives are: , In a convex set, the system matrix There are the following relationships: , in, represents a convex set, is the system matrix Middle Line The convex set of column elements is calculated as follows: , in, Representation matrix Middle Line Nominal values ​​of column elements; orthogonal matrix and the diagonal matrix Obtained by Cholesky decomposition: ; represents the hyperellipsoid formed by the initial convex set uncertainty parameters; yes Bias vector for each uncertainty parameter: ; express Convex set perturbation of ; Through convex set uncertainty, we know The boundary of is calculated by the following formula: , In step 4, the uncertainty range of the system matrix and the input matrix is: 。 9. A method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 8, characterized in that: In step 5, the system response function under unit pulse excitation is for: , Construct the generalized Hankel matrix as: , in, and They represent the number of row blocks and column blocks of the generalized Hankel matrix respectively; In step 5, the partial derivative of the generalized Hankel matrix with respect to the uncertainty parameter is calculated: , in, .

10. A method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 9, characterized in that: In step 6, the generalized Hankel matrix considering parameter correlation is Perform a second-order singular value decomposition: , in, denote the left singular value matrix and the right singular value matrix respectively, Respectively represent Column left singular value vector and Column right singular value vector: , in, is the mode number of interest; , , They represent the center value of the left singular value vector and the uncertainty range of the left singular value vector after the first-order and second-order Taylor expansion respectively; , , They represent the central value of the right singular value vector and the uncertainty range of the right singular value vector after the first-order and second-order Taylor expansion respectively; is the singular value matrix, Indicates singular values; , where , , They represent the central value of the singular value and the uncertainty range of the singular value after the first-order and second-order Taylor expansion respectively; The radius after the first-order Taylor expansion is calculated by the following formula: , in, express Bias vector for each uncertainty parameter: , express Bias vector for each uncertainty parameter: , express Bias vector for each uncertainty parameter: , The uncertainty range after the second-order Taylor expansion is calculated by the following formula: , According to the propagation of convex set uncertainty, we have: , in, They represent the partial derivative of the left singular value vector with respect to the uncertainty parameter and the partial derivative of the right singular value vector with respect to the interval uncertainty parameter, respectively, and are calculated by the following formula: , in, Indicates The left singular value vector elements, Indicates The right singular value vector elements.

11. The method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 9, characterized in that: In step 7, the generalized Hankel matrix after time elapses is for: 。 12. A method for identifying modal parameters of a structure with bounded and correlated uncertainties according to claim 11, characterized in that: In step 8, the structure recognition system matrix constructed for: , in, ; Structure Identification System Matrix The partial derivative with respect to the uncertainty parameter is: 。 13. A method for identifying modal parameters of a structure with bounded and correlated uncertainties according to claim 12, characterized in that: In step 9, the structure identification system matrix The second-order convex set eigenvalue decomposition is: , in, is the eigenvalue vector, represents the complex eigenvalue matrix, Indicates Item complex eigenvalue; , , , Among them, the first-order partial derivative of the complex eigenvalue with respect to the uncertainty parameter And the second-order partial derivative It is calculated as follows: , , Among them, the first-order partial derivative of the eigenvalue vector with respect to the uncertainty parameter for: , 。 14. A method for modal parameter identification of a structure with bounded and correlated uncertainties according to claim 13, characterized in that: In step 10, the modal parameters of the structure calculated are: Natural circular frequency for: , in, They represent the central value of the natural frequency, the uncertainty range of the natural frequency, and the lower and upper limits of the range, respectively. The expression is ; The upper and lower bounds are determined as follows: Will The expression is regarded as The quadratic function of is a variable with a range, we get exist The minimum and maximum values ​​within the range of variation are the lower and upper bounds, and the calculation process is as follows: , , in, represents the uncertainty parameter of the i-th natural frequency with respect to the j-th uncertainty parameter The uncertainty range of Among them, the first-order and second-order partial derivatives of the natural circular frequency with respect to the uncertainty parameter are as follows: , , in, Represents complex eigenvalues The partial derivatives of the real and imaginary parts of the uncertainty parameter are calculated by the following formula: , , Damping ratio range for: ; in, They represent the central value of the damping ratio, the uncertainty range of the damping ratio, and the lower and upper bounds, respectively. The expression is ; The upper and lower bounds are determined as follows: Will The expression is regarded as The quadratic function of is a variable with a range, we get exist The minimum and maximum values ​​within the range of variation are the lower and upper bounds, and the calculation process is as follows: , , in, represents the uncertainty parameter of the i-th natural frequency with respect to the j-th uncertainty parameter The uncertainty range of Among them, the first-order and second-order partial derivatives of the damping ratio with respect to the uncertainty parameter are as follows: , 。

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